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{{short description|Class of hypothetical redshift mechanisms}} |
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{{cosmology}} |
{{cosmology}} |
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'''Tired light''' is a class of hypothetical [[redshift]] mechanisms that was proposed as an alternative explanation for the [[Hubble's law|redshift-distance relationship]] |
'''Tired light''' is a class of hypothetical [[redshift]] mechanisms that was proposed as an alternative explanation for the [[Hubble's law|redshift-distance relationship]]. These models have been proposed as alternatives to the models that involve the [[expansion of the universe]]. The concept was first proposed in 1929 by [[Fritz Zwicky]], who suggested that if photons lost energy over time through collisions with other particles in a regular way, the more distant objects would appear redder than more nearby ones. |
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Zwicky acknowledged that any sort of [[scattering]] of light would blur the images of distant objects more than what is seen. Additionally, the [[Tolman surface brightness test|surface brightness of galaxies evolving with time]], [[time dilation]] of cosmological sources, and a thermal spectrum of the [[cosmic microwave background]] have been observed—these effects should not be present if the cosmological redshift was due to any tired light scattering mechanism.<ref name="nedwright">[[Ned Wright|Wright, E. L.]] ''[http://www.astro.ucla.edu/~wright/tiredlit.htm Errors in Tired Light Cosmology]''.</ref><ref name="treu" /><ref name="Peebles"> |
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== History and reception == |
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{{Cite book |
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{{See also|Redshift|Non-standard cosmologies#Static Universe Models}} |
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|last1=Peebles|first1 = P. J. E. |
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Tired [[light]] was an idea that came about due to the observation made by [[Edwin Hubble]] that [[galaxy|distant galaxies]] have [[redshift]]s proportional to their [[distance measures (cosmology)|distance]]. Redshift is a shift in the spectrum of [[electromagnetic radiation]] toward lower energies and frequencies, usually attributed to [[recessional velocity]]. Before Hubble's observations, all observed redshifts were attributable directly to a mechanism similar to the [[Doppler Effect]]. In these situations, objects moving away from us exhibit a shift toward the red end of the [[optical spectrum]] while objects moving toward us exhibit a shift toward the blue end ([[blueshift]]). Hubble and other scientists observing the redshifts associated with distant galaxies attributed their redshifts to motion away from us. Bizarrely, the relation held in all directions and so could not be attributed to normal movement with respect to a background which would show redshifts and blueshifts. Everything was moving ''away''. |
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|year=1998 |
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|chapter=The Standard Cosmological Model |
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|editor-last=Greco |editor-first=M. |
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|title=Rencontres de Physique de la Vallee d'Aosta |
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|arxiv = astro-ph/9806201 |
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}}</ref> Despite periodic re-examination of the concept, tired light has not been supported by observational tests and remains a [[fringe physics|fringe topic]] in astrophysics.<ref name="overduin-2008"> |
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{{cite book |
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|first1=James Martin |last1=Overduin |
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|first2=Paul S. |last2=Wesson |
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|year=2008 |
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|title=The light/dark universe: light from galaxies, dark matter and dark energy |
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|page=10 |
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|publisher=World Scientific Publishing |
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|isbn=978-981-283-441-6 |
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}}</ref> |
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==History and reception== |
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Immediately upon publishing these results, [[Willem de Sitter]] who was working with [[Einstein]]'s [[Theory of General Relativity]] recognized that these observations fit with a particular solution to the [[Einstein equations]] now known as the [[FRW metric]]. This solution explains that distant objects are observed with greater wavelengths than were emitted by the objects because they are moving with an [[expansion of the universe]]. In this formulation, there was still an analogous effect to the [[Doppler Effect]], though relative velocities are not really well-defined for such situations. |
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{{See also|Redshift|Non-standard cosmology#Tired light}} |
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Tired [[light]] was an idea that came about due to the observation made by [[Edwin Hubble]] that [[galaxy|distant galaxies]] have [[redshift]]s proportional to their [[distance measures (cosmology)|distance]]. Redshift is a shift in the [[astronomical spectroscopy|spectrum]] of the emitted [[electromagnetic radiation]] from an object toward lower energies and frequencies, associated with the phenomenon of the [[Doppler effect]]. Observers of [[spiral nebula]]e such as [[Vesto Slipher]] observed that these objects (now known to be separate [[galaxy|galaxies]]) generally exhibited redshift rather than blueshifts independent of where they were located. Since the relation holds in all directions it cannot be attributed to normal movement with respect to a background which would show an assortment of redshifts and blueshifts. Everything is moving ''away'' from the Milky Way galaxy. Hubble's contribution was to show that the magnitude of the redshift correlated strongly with the distance to the galaxies. |
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Basing on Slipher's and Hubble's data, in 1927 [[Georges Lemaître]] realized that this correlation could fit non-static solutions to the equations of Einstein's theory of gravity, the Friedmann–Lemaître solutions. However Lemaître's article was appreciated only after Hubble's publication of 1929. The universal redshift-distance relation in this solution is attributable to the effect an expanding universe has on a photon traveling on a null [[spacetime interval]] (also known as a "light-like" [[geodesic]]). In this formulation, there was still an analogous effect to the [[Doppler effect]], though relative velocities need to be handled with more care since [[comoving distance|distances]] can be defined in different ways in [[expansion of the universe|an expanding universe]]. |
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Not everyone accepted this interpretation immediately. General relativity was notoriously difficult to understand and many of the astronomers were skeptical that this was the only possible explanation. Some, like [[Edward Milne]] proposed that there was a giant explosion that could explain redshifts (see [[Milne universe]]). Others thought that there might be [[systematics|systematic effects]] that made the observation suspect. Along this line, [[Fritz Zwicky]] proposed a "tired light" mechanism in 1929.<ref name="Zwicky">Zwicky, F. 1929. ''On the Red Shift of Spectral Lines through Interstellar Space.'' PNAS '''15''':773-779. [http://adsabs.harvard.edu/cgi-bin/nph-bib_query?1929PNAS...15..773Z Abstract] (ADS) [http://www.pnas.org/cgi/reprintframed/15/10/773 Full article] (PDF)</ref> Zwicky suggested that [[photon]]s might slowly lose [[energy]] as they travel vast [[distance]]s through a [[static universe]] by interaction with matter or other photons, or by some novel physical mechanism. Since a decrease in [[energy]] corresponds to an increase in light's [[wavelength]], this effect would produce a [[redshift]] in [[spectral line]]s that increase [[Proportionality (mathematics)|proportionally]] with the distance of the source. The term "tired light" was coined by [[Richard Tolman]] in the early 1930s as a way to refer to this idea.<ref>{{cite book |last1=Evans |first1=Myron W. |last2=Vigier |first2=Jean-Pierre |title=The Enigmatic Photon: Theory and Practice of the B3 Field |url=http://books.google.com/?id=2-0p1eOCYeIC&pg=PA29&lpg=PA29&dq=%22tired+light%22+coined+tolman |page=29 |publisher=Springer |year=1996 |isbn=0792340442}}</ref> |
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At the same time, other explanations were proposed that did not concord with general relativity. [[Edward Arthur Milne|Edward Milne]] proposed an explanation compatible with [[special relativity]] but not general relativity that there was a giant explosion that could explain redshifts (see [[Milne universe]]). Others proposed that [[systematics|systematic effects]] could explain the redshift-distance correlation. Along this line, [[Fritz Zwicky]] proposed a "tired light" mechanism in 1929.<ref name="Zwicky">{{Cite journal |doi = 10.1073/pnas.15.10.773|pmid = 16577237|pmc = 522555|bibcode = 1929PNAS...15..773Z|title = On the Redshift of Spectral Lines Through Interstellar Space|year = 1929|last1 = Zwicky|first1 = F.|journal = Proceedings of the National Academy of Sciences|volume = 15|issue = 10|pages = 773–779|doi-access = free}}</ref> Zwicky suggested that [[photon]]s might slowly lose [[energy]] as they travel vast [[distance]]s through a [[static universe]] by interaction with matter or other photons, or by some novel physical mechanism. Since a decrease in [[energy]] corresponds to an increase in light's [[wavelength]], this effect would produce a [[redshift]] in [[spectral line]]s that increase [[Proportionality (mathematics)|proportionally]] with the distance of the source. The term "tired light" was coined by [[Richard Tolman]] in the early 1930s as a way to refer to this idea.<ref>{{cite book |last1=Evans |first1=Myron W. |last2=Vigier |first2=Jean-Pierre |title=The Enigmatic Photon: Theory and Practice of the B3 Field |url=https://books.google.com/books?id=2-0p1eOCYeIC&q=%22tired+light%22+coined+tolman&pg=PA29 |page=29 |publisher=Springer |date=1996 |isbn=978-0-7923-4044-7}}</ref> [[Helge Kragh]] has noted "Zwicky’s hypothesis was the best known and most elaborate alternative to the expanding universe, but it was far from the only one. More than a dozen physicists, astronomers and amateur scientists proposed in the 1930s tired-light ideas having in common the assumption of nebular photons interacting with intergalactic matter to which they transferred part of their energy." Kragh noted in particular [[John Quincy Stewart]], [[William Duncan MacMillan]], and [[Walther Nernst]].<ref>{{cite book |editor1-first=Helge |editor1-last=Kragh |editor2-first=Malcolm S. |editor2-last=Longair |title=The Oxford Handbook of the History of Modern Cosmology |date=2019 |chapter=Alternative Cosmological Theories |first=Helge |last=Kragh |doi=10.1093/oxfordhb/9780198817666.013.4 |page=29|isbn=978-0-19-881766-6 }}</ref> |
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Tired light mechanisms were among the proposed alternatives to the [[Big Bang]] and the [[Steady State Theory|Steady State]] [[physical cosmology|cosmologies]], both of which relied on the general relativistic expansion of the universe of the FRW metric. Through the middle of the twentieth century, most cosmologists supported one of these two [[paradigm]]s, but there were a few scientists who worked with the tired light alternative.<ref>Wilson, O. C. 1939. ''Possible applications of supernovae to the study of the nebular red shifts.'' Astrophysical Journal '''90''':634-636. [http://adsabs.harvard.edu/cgi-bin/bib_query?1939ApJ....90..634W Archived article (ADS)]</ref> As the discipline of [[observational cosmology]] developed in the late twentieth century and the associated data became more numerous and accurate, the Big Bang emerged as the cosmological theory most supported by the observational evidence, and it remains the accepted [[scientific consensus|consensus model]] in the current [[Lambda-CDM model|parametrization]] of the state and evolution of the universe. Additionally, a number of studies have shown that the traditional "tired light" hypothesis is not a viable explanation for cosmological redshifts. One of the reasons is that in an static universe, the surface brightness of stars and galaxies should be constant, that is, the farther an object is, the less light we receive, but its apparent area diminishes as well, so the light received divided by the apparent area should be constant. In an expanding universe, the surface brightness diminishes with distance. As the observed object recedes, photons are emitted at a reduced rate because each photon has to travel a distance that is a little longer than the previous one, while its energy is reduced a little because of increasing redshift at a larger distance. On the other hand, in an expanding Universe, the object appears to be larger than it really is, because it was closer to us when the photons started their travel. This causes a difference in surface brilliance of objects between a static and an expanding Universe. This allows us to produce a test known as the [[Tolman surface brightness test]] that in those studies favors an expanding Universe hypothesis.<ref name = "Geller">Geller J. et al.,[http://articles.adsabs.harvard.edu/cgi-bin/nph-iarticle_query?1972ApJ...174....1G&data_type=PDF_HIGH&type=PRINTER&filetype=.pdf Test of the expanding universe postulate] The astrophysical journal 174, p.1 (1972)</ref><ref>[[Gerson Goldhaber|Goldhaber]], et al. (2001) Timescale Stretch Parameterization of Type Ia Supernova B-band Light Curves [http://arxiv.org/abs/astro-ph/0104382 url]</ref><ref>Lubin and Sandage(2001), The Tolman Surface Brightness Test for the Reality of the Expansion. IV. A Measurement of the Tolman Signal and the Luminosity Evolution of Early-Type Galaxies, [http://arxiv.org/abs/astro-ph/0106566 url]</ref> |
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Tired light mechanisms were among the proposed alternatives to the [[Big Bang]] and the [[Steady State Theory|Steady State]] [[physical cosmology|cosmologies]], both of which relied on the general relativistic expansion of the universe of the FRW metric. Through the middle of the twentieth century, most cosmologists supported one of these two [[paradigm]]s, but there were a few scientists, especially those who were working on alternatives to general relativity, who worked with the tired light alternative.<ref>{{Cite journal |bibcode = 1939ApJ....90..634W|title = Possible Applications of Supernovae to the Study of the Nebular Red Shifts|last1 = Wilson|first1 = O. C.|journal = The Astrophysical Journal|volume = 90|pages = 634|year = 1939|doi = 10.1086/144134}}</ref> As the discipline of [[observational cosmology]] developed in the late twentieth century and the associated data became more numerous and accurate, the Big Bang emerged as the cosmological theory most supported by the observational evidence, and it remains the accepted [[scientific consensus|consensus model]] with a current [[Lambda-CDM model|parametrization]] that precisely specifies the state and evolution of the universe. Although the proposals of "tired light cosmologies" are now more-or-less relegated to the dustbin of history, as a completely alternative proposal tired-light cosmologies were considered a remote possibility worthy of some consideration in cosmology texts well into the 1980s, though it was dismissed as an unlikely and ''ad hoc'' proposal by mainstream astrophysicists.<ref>See, for example, p. 397 of [[Joseph Silk]]'s book, ''The Big Bang''. (1980) W. H. Freeman and Company. {{ISBN|0-7167-1812-X}}.</ref> |
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Redshift is directly observable and used by cosmologists as a direct measure of [[time]]. They often refer to age in terms of redshift rather than years. The [[Big Bang]] is the end of this scale of time that corresponds to a redshift of infinity. The [[Hubble's Law|relation between universal expansion and redshift]] is observationally confirmed through a variety of tests, though alternative hypotheses such as tired light remain historically interesting and cannot be completely ruled out, as the underlying mechanism can be adjusted to observations or embellished in a similar way as many competing expanding Universe hypotheses have been fitted to observational data.<ref name="Geller" /> [[Alternative theories of gravity]] that do not have an expanding universe in them need an alternative to explain the correspondence between redshift and distance that is ''[[sui generis]]'' to the [[Metric expansion of space|expanding metrics]] of general relativity. Such theories are sometimes referred to as "tired-light cosmologies", though not all authors are necessarily aware of the historical antecedents.<ref>{{cite book |last=Barrow |first=John D. |title=The Routledge Companion to the New Cosmology |editor=Peter Coles |publisher=Routledge |year=2001 |isbn=0-415-24312-2 |page=308}}</ref> |
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[[File:Tolman_surface_brightness_test.png|thumb|upright=1.5|The Tolman surface brightness test rules out the tired light explanation for the cosmological redshift.]] |
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==Tired light models== |
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By the 1990s and on into the twenty-first century, a number of falsifying observations have shown that "tired light" hypotheses are not viable explanations for cosmological redshifts.<ref name="treu">Tommaso Treu, Lecture slides for [[University of California at Santa Barbara]] Astrophysics course. [http://www.physics.ucsb.edu/~tt/ASTRO2/lecture16.pdf p. 16]. {{Webarchive|url=https://web.archive.org/web/20100623125705/http://www.physics.ucsb.edu/~tt/ASTRO2/lecture16.pdf|date=2010-06-23}}.</ref> For example, in a static universe with tired light mechanisms, the surface brightness of stars and galaxies should be constant, that is, the farther an object is, the less light we receive, but its apparent area diminishes as well, so the light received divided by the apparent area should be constant. In an expanding universe, the surface brightness diminishes with distance. As the observed object recedes, photons are emitted at a reduced rate because each photon has to travel a distance that is a little longer than the previous one, while its energy is reduced a little because of increasing redshift at a larger distance. On the other hand, in an expanding universe, the object appears to be larger than it really is, because it was closer to us when the photons started their travel. This causes a difference in surface brilliance of objects between a static and an expanding Universe. This is known as the [[Tolman surface brightness test]] that in those studies favors the expanding universe hypothesis and rules out static tired light models.<ref name = "Geller">{{Cite journal |bibcode = 1972ApJ...174....1G|title = Test of the Expanding Universe Postulate|last1 = Geller|first1 = M. J.|last2 = Peebles|first2 = P. J. E.|journal = The Astrophysical Journal|volume = 174|pages = 1|year = 1972|doi = 10.1086/151462|doi-access = free}}</ref><ref>{{cite journal|last1=Goldhaber|first1=G.|last2=Groom|first2=D. E.|last3=Kim|first3=A.|last4=Aldering|first4=G.|last5=Astier|first5=P.|last6=Conley|first6=A.|last7=Deustua|first7=S. E.|last8=Ellis|first8=R.|last9=Fabbro|first9=S.|last10=Fruchter|first10=A. S.|last11=Goobar|first11=A.|last12=Hook|first12=I.|last13=Irwin|first13=M.|last14=Kim|first14=M.|last15=Knop|first15=R. A.|last16=Lidman|first16=C.|last17=McMahon|first17=R.|last18=Nugent|first18=P. E.|last19=Pain|first19=R.|last20=Panagia|first20=N.|last21=Pennypacker|first21=C. R.|last22=Perlmutter|first22=S.|last23=Ruiz-Lapuente|first23=P.|last24=Schaefer|first24=B.|last25=Walton|first25=N. A.|last26=York|first26=T.|author27=The Supernova Cosmology Project|title=Timescale Stretch Parameterization of Type Ia Supernova B-band Light Curves|doi=10.1086/322460|date=2001|journal=The Astrophysical Journal|volume=558|issue=1|pages=359–368|arxiv=astro-ph/0104382|bibcode = 2001ApJ...558..359G |s2cid=17237531}}</ref><ref>{{Cite journal |arxiv = astro-ph/0106566|doi = 10.1086/322134|bibcode = 2001AJ....122.1084L|title = The Tolman Surface Brightness Test for the Reality of the Expansion. IV. A Measurement of the Tolman Signal and the Luminosity Evolution of Early-Type Galaxies|year = 2001|last1 = Lubin|first1 = Lori M.|last2 = Sandage|first2 = Allan|journal = The Astronomical Journal|volume = 122|issue = 3|pages = 1084–1103|s2cid = 118897528}}</ref> |
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A number of tired light mechanisms have been suggested over the years: |
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Redshift is directly observable and used by cosmologists as a direct measure of [[cosmological time|lookback time]]. They often refer to age and distance to objects in terms of redshift rather than years or light-years. In such a scale, the [[Big Bang]] corresponds to a redshift of infinity.<ref name="Geller" /> [[Alternative theories of gravity]] that do not have an expanding universe in them need an alternative to explain the correspondence between redshift and distance that is ''[[sui generis]]'' to the [[Metric expansion of space|expanding metrics]] of general relativity. Such theories are sometimes referred to as "tired-light cosmologies", though not all authors are necessarily aware of the historical antecedents.<ref>{{cite book |last=Barrow |first=John D. |title=The Routledge Companion to the New Cosmology |editor=Peter Coles |publisher=Routledge |date=2001 |isbn=978-0-415-24312-4 |page=308|bibcode=2001rcnc.book.....C }}</ref> |
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===Zwicky's models=== |
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==Specific falsified models== |
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[[Fritz Zwicky]] investigated a number of redshift explanations, ruling out some himself: |
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[[Image:Hubble ultra deep field high rez edit1.jpg|thumb|right|upright=1.5| The [[Hubble Ultra Deep Field]] is an image of galaxies that are in excess of 10 billion light years away. If tired light was a correct explanation, these galaxies would appear blurred in comparison to closer galaxies. That they do not rules out the suggestion that scattering processes are causing the redshift-distance relation.]] |
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In general, any "tired light" mechanism must solve some basic problems, in that the observed redshift must: |
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*admit the same measurement in any wavelength-band |
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*not exhibit blurring |
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*follow the detailed Hubble relation observed with [[supernova]] data (see [[accelerating universe]]) |
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*explain associated [[time dilation]] of cosmologically distant events. |
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A number of tired light mechanisms have been suggested over the years. [[Fritz Zwicky]], in his paper proposing these models investigated a number of redshift explanations, ruling out some himself. The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled:<math display="block">E(x)=E_0 \exp\left(-\frac{x}{R_0}\right)</math>where <math>E(x)</math> is the energy of the photon at distance <math>x</math> from the source of light, <math>E_0</math> is the energy of the photon at the source of light, and <math>R_0</math> is a large constant characterizing the "resistance of the space". To correspond to [[Hubble's law]], the constant <math>R_0</math> must be several giga[[parsec]]s. <!--It must be large enough to take into account any deviation from Hubble's law--> For example, Zwicky considered whether an integrated [[Compton effect]] could account for the scale normalization of the above model: |
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*'''The Compton Effect''': |
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{{ |
{{blockquote|... light coming from distant nebulae would undergo a shift to the red by [[Compton effect]] on those free electrons [in interstellar spaces] [...] But then the light scattered in all directions would make the interstellar space intolerably opaque which disposes of the above explanation. [...] it is evident that any explanation based on a scattering process like the Compton effect or the [[Raman effect]], etc., will be in a hopeless position regarding the good definition of the images.<ref name="Zwicky" />}} |
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This expected "blurring" of cosmologically distant objects is not seen in the observational evidence, though it would take much larger telescopes than those available at that time to show this with certainty. Alternatively, Zwicky proposed a kind of [[Sachs–Wolfe effect]] explanation for the redshift distance relation: |
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*'''Gravitational potential''': |
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{{ |
{{blockquote|One might expect a shift of spectral lines due to the difference of the static gravitational potential at different distances from the center of a galaxy. This effect, of course, has no relation to the distance of the observed galaxy from our own system and, therefore, cannot provide any explanation of the phenomenon discussed in this paper.<ref name="Zwicky" />}} |
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Zwicky's proposals were carefully presented as falsifiable according to later observations: |
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*'''The Gravitational "Drag" of Light''': |
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{{ |
{{blockquote|... [a] gravitational analogue of the Compton effect [...] It is easy to see that the above redshift should broaden these absorption lines asymmetrically toward the red. If these lines can be photographed with a high enough dispersion, the displacement of the center of gravity of the line will give the redshift independent of the velocity of the system from which the light is emitted.<ref name="Zwicky" />}} |
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Such broadening of absorption lines is not seen in high-redshift objects, thus falsifying this particular hypothesis.<ref>{{Cite web |last=Newton |first=Elisabeth |date=27 April 2011 |title=Prospecting for C IV at high redshifts |url=https://astrobites.org/2011/04/27/prospecting-for-c-iv-at-high-redshifts/ |access-date=4 November 2023 |website=[[astrobites.org]]}}</ref> |
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Zwicky also notes, in the same paper, that according to a tired light model a distance-redshift relationship would necessarily be present in the light from sources within our own galaxy (even if the redshift would be so small that it would be hard to measure), that do not appear under a recessional-velocity based theory. He writes, referring to sources of light within our galaxy: "It is especially desirable to determine the redshift independent of the proper velocities of the objects observed".<ref name="Zwicky" /> |
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Zwicky also notes, in the same paper, that according to a tired light model a distance-redshift relationship would necessarily be present in the light from sources within our own galaxy (even if the redshift would be so small that it would be hard to measure), that do not appear under a recessional-velocity based theory. He writes, referring to sources of light within our galaxy: "It is especially desirable to determine the redshift independent of the proper velocities of the objects observed".<ref name="Zwicky" /> Subsequent to this, astronomers have patiently mapped out the three-dimensional velocity-position [[phase space]] for the galaxy and found the redshifts and blueshifts of galactic objects to accord well with the statistical distribution of a spiral galaxy, eliminating the [[intrinsic redshift]] component as an effect.<ref>Binney & Merrifield: ''Galactic Astronomy''. Princeton University Press, {{ISBN|978-0-691-02565-0}}.</ref> |
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===Hubble and Tolman's "energy loss" treatment=== |
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Following after Zwicky in 1935, [[Edwin Hubble]] and [[Richard Tolman]] compare recessional redshift with a non-recessional one, writing that they: |
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{{quote|... both incline to the opinion, however, that if the red-shift is not due to recessional motion, its explanation will probably involve some quite new physical principles [... and] use of a static Einstein model of the universe, combined with the assumption that the photons emitted by a nebula lose energy on their journey to the observer by some unknown effect, which is linear with distance, and which leads to a decrease in frequency, without appreciable transverse deflection.<ref>{{cite journal |last1=Hubble |first1=Edwin |last2=Tolman |first2=Richard C. |authorlink1=Edwin Hubble |authorlink2=Richard C. Tolman |title=Two Methods of Investigating the Nature of the Nebular Redshift |date=11/1935 |journal=Astrophysical Journal |volume=82 |page=302 |doi=10.1086/143682 |bibcode=1935ApJ....82..302H}}</ref>}} |
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Following after Zwicky in 1935, [[Edwin Hubble]] and [[Richard Tolman]] compared recessional redshift with a non-recessional one, writing that they |
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===Finlay-Freundlich Red Shift Hypothesis=== |
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In the early 1950s, [[Erwin Finlay-Freundlich]] proposed a redshift as "the result of loss of energy by observed photons traversing a radiation field."<ref name="finlay">{{cite journal | last1 = Finlay-Freundlich | first1 = E. | year = 1954 | title = Red-Shifts in the Spectra of Celestial Bodies | url = http://www.iop.org/EJ/abstract/0370-1298/67/2/114 | journal = Proc. Phys. Soc. A | volume = 67 | issue = 2| pages = 192–193 | doi = 10.1088/0370-1298/67/2/114 |bibcode = 1954PPSA...67..192F }}</ref> R.A. Alpher noted, "No generally accepted physical mechanism has been proposed for this loss,"<ref>{{cite journal | last1 = Alpher | first1 = R.A. | year = 1962 | title = Laboratory Test of the Finlay-Freundlich Red Shift Hypothesis | url = http://www.nature.com/nature/journal/v196/n4852/abs/196367b0.html | journal = Nature | volume = 196 | issue = 4852| pages = 367–368 | doi=10.1038/196367b0|bibcode = 1962Natur.196..367A }}</ref> though P.F. Brown "... proposed that the energy lost reappears as neutrino pairs resulting from the exchange of a graviton between two photons."<ref>{{cite journal | last1 = Brown | first1 = P.F. | year = 1962 | title = The Case for an Exponential Red Shift Law | url = http://www.nature.com/nature/journal/v193/n4820/abs/1931019a0.html | journal = Nature | volume = 193 | issue = 4820| pages = 1019–1021 | doi=10.1038/1931019a0|bibcode = 1962Natur.193.1019B }}</ref> |
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{{blockquote|both incline to the opinion, however, that if the red-shift is not due to recessional motion, its explanation will probably involve some quite new physical principles [... and] use of a static Einstein model of the universe, combined with the assumption that the photons emitted by a nebula lose energy on their journey to the observer by some unknown effect, which is linear with distance, and which leads to a decrease in frequency, without appreciable transverse deflection.<ref>{{cite journal |last1=Hubble |first1=Edwin |last2=Tolman |first2=Richard C. |authorlink1=Edwin Hubble |authorlink2=Richard C. Tolman |title=Two Methods of Investigating the Nature of the Nebular Redshift |date=November 1935 |journal=Astrophysical Journal |volume=82 |page=302 |doi=10.1086/143682 |bibcode=1935ApJ....82..302H}}</ref>}} These conditions became almost impossible to meet and the overall success of general relativistic explanations for the redshift-distance relation is one of the core reasons that the Big Bang model of the universe remains the cosmology preferred by researchers. |
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==General features of tired light models== |
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The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled: |
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In the early 1950s, [[Erwin Finlay-Freundlich]] proposed a redshift as "the result of loss of energy by observed photons traversing a radiation field".<ref name="finlay">{{cite journal | last1 = Finlay-Freundlich | first1 = E. | date = 1954 | title = Red-Shifts in the Spectra of Celestial Bodies | journal = Proceedings of the Physical Society A | volume = 67 | issue = 2| pages = 192–193 | doi = 10.1088/0370-1298/67/2/114 |bibcode = 1954PPSA...67..192F }}</ref> which was cited and argued for as an explanation for the redshift-distance relation in a 1962 astrophysics theory ''[[Nature (journal)|Nature]]'' paper by [[University of Manchester]] physics professor P. F. Browne.<ref>{{cite journal | last1 = Brown | first1 = P. F. | date = 1962 | title = The Case for an Exponential Red Shift Law | journal = Nature | volume = 193 | issue = 4820| pages = 1019–1021 | doi=10.1038/1931019a0|bibcode = 1962Natur.193.1019B | s2cid = 4154001 }}</ref> The pre-eminent cosmologist [[Ralph Asher Alpher]] wrote a letter to ''Nature'' three months later in response to this suggestion heavily criticizing the approach, "No generally accepted physical mechanism has been proposed for this loss."<ref>{{cite journal | last1 = Alpher | first1 = R. A. | date = 1962 | title = Laboratory Test of the Finlay-Freundlich Red Shift Hypothesis | journal = Nature | volume = 196 | issue = 4852| pages = 367–368 | doi=10.1038/196367b0|bibcode = 1962Natur.196..367A | s2cid = 4197527 }}</ref> Still, until the so-called "Age of Precision Cosmology" was ushered in with results from the [[WMAP]] space probe and modern [[redshift survey]]s,<ref>[[George Smoot|Smoot, George S.]] "Our Age of Precision Cosmology". Proceedings of the 2002 International Symposium on Cosmology and Particle Astrophysics (CosPA 02), Taipei, Taiwan, 31 May – 2 June 2002, pp. 314–325.</ref> tired light models could occasionally get published in the mainstream journals, including one that was published in the February 1979 edition of ''Nature'' proposing "photon decay" in a curved spacetime<ref>{{cite journal |first=D. F. |last=Crawford |title=Photon Decay in Curved Space-time |journal=[[Nature (journal)|Nature]] |volume=277 |issue=5698 |pages=633–635 |year=1979|doi=10.1038/277633a0 |bibcode=1979Natur.277..633C |s2cid=4317887 }}</ref> that was five months later criticized in the same journal as being wholly inconsistent with observations of the [[gravitational redshift]] observed in the [[limb darkening|solar limb]].<ref>{{cite journal |last1= Beckers |first1=J. M. |last2 = Cram |first2=L. E. |title = Use of the solar limb effect to test photon decay and cosmological redshift theories |journal = [[Nature (journal)|Nature]] |date=July 1979 |volume = 280 |issue = 5719 |pages = 255–256 |doi = 10.1038/280255a0 |bibcode = 1979Natur.280..255B|s2cid=43273035 }}</ref> In 1986, a paper claiming tired light theories explained redshift better than cosmic expansion was published in the ''Astrophysical Journal'',<ref>{{cite journal|last=LaViolette |first=P. A. |title=Is the universe really expanding? |journal=Astrophysical Journal |date=April 1986 |volume=301 |pages=544–553|bibcode = 1986ApJ...301..544L |doi = 10.1086/163922 }}</ref> but ten months later, in the same journal, such tired light models were shown to be inconsistent with extant observations.<ref>{{cite journal|last=Wright |first=E. L.|author-link=Ned Wright|title=Source counts in the chronometric cosmology|journal=Astrophysical Journal|date=February 1987|volume=313|pages=551–555|bibcode = 1987ApJ...313..551W|doi =10.1086/164996 }}</ref> As cosmological measurements became more precise and the statistics in cosmological data sets improved, tired light proposals ended up being falsified,<ref name=nedwright /><ref name=treu /><ref name=Peebles /> to the extent that the theory was described in 2001 by science writer [[Charles Seife]] as being "firmly on the [[fringe physics|fringe of physics]] 30 years ago; still, scientists sought more direct proofs of the expansion of the cosmos".<ref name="Seife">{{cite news |author=Seife |first=Charles |author-link=Charles Seife |date=28 June 2001 |title='Tired-Light' Hypothesis Gets Re-Tired |url=https://www.science.org/content/article/tired-light-hypothesis-gets-re-tired |accessdate=2016-06-03 |work=[[Science (journal)|Science]] |quote=Measurements of the cosmic microwave background put the theory firmly on the fringe of physics 30 years ago; still, scientists sought more direct proofs of the expansion of the cosmos.}}</ref> |
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:<math>E(x)=E(0)e^{-\frac{x}{R}}</math> |
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==See also== |
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where ''E(x)'' is the energy of the photon at distance ''x'' from the source of light, ''E(0)'' is the energy of the photon at the source of light, and ''R'' is a large constant characterizing the "resistance of the space". To correspond to [[Hubble's law]], the constant ''R'' must be several giga[[parsec]]s. <!--It must be large enough to take into account any deviation from Hubble's law--> |
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* [[Dispersion (optics)]] |
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== |
==References== |
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{{Reflist}} |
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Any "tired light" mechanism must solve some basic problems, in that the observed redshift must: |
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*admit the same measurement in any wavelength-band |
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*not exhibit blurring |
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*follow the detailed Hubble relation observed with [[supernova]] data (see [[accelerating universe]]) |
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*explain associated [[time dilation]] of cosmologically distant events.<ref>While supernova light curve data are consistent with time dilation and rule out some static cosmologies, a 2010 comparison of quasar light curves at high and low redshifts did not show the expected evidence of time dilation, see {{cite journal |
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| last = Hawkins |
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| first = M. R. S. |
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| date = 9 April 2010 |
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| title = On time dilation in quasar light curves |
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| journal = Monthly Notices of the Royal Astronomical Society |
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| issn = 1365-2966 |
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| doi = 10.1111/j.1365-2966.2010.16581.x |
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| accessdate = 19 April 2010 |
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| quote = In this paper we set out to measure time dilation in quasar light curves. In order to detect the effects of time dilation, sets of light curves from two monitoring programmes are used to construct Fourier power spectra covering time-scales from 50 d to 28 yr. Data from high- and low-redshift samples are compared to look for the changes expected from time dilation. The main result of the paper is that quasar light curves do not show the effects of time dilation. |
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| bibcode=2010MNRAS.405.1940H |
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}}</ref> |
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As part of a broader [[non-standard cosmology|alternative cosmology]], other observations that need explanation include: |
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*the detail observations of the [[cosmic microwave background radiation]] |
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*[[Big Bang nucleosynthesis|the abundance of light elements]] |
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*[[Large-scale structure of the cosmos|large-scale structure statistics]] |
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To date, no established mechanism to produce such a drop in energy has been proposed that reproduces all the observations associated with the redshift—distance relation. [[Scattering]] by known mechanisms from gas or dust does not reproduce the observations. For example, scattering by any mechanism would blur an object more than observed. In general, cosmologists consider classical tired light models to have too many problems to be worth serious consideration.<ref>[[Edward L. Wright|Ned Wright]]; [http://www.astro.ucla.edu/~wright/tiredlit.htm ''Errors in Tired Light Cosmology''] (2005)</ref> Tired light alone does not provide a full cosmological explanation and so cannot reproduce all the successes of the standard [[big bang]] cosmology. No tired light theory is known that by itself correctly accounts for the observed time dilation of distant [[supernova]]e light curves,<ref>Wilson, 1939 and [[Gerson Goldhaber|Goldhaber]], 2001.</ref> the black body spectrum or anisotropy of the [[cosmic microwave background]], and the observed change in the morphology, number count, and surface brightness of high redshift [[galaxy|galaxies]] and [[quasar]]s. Furthermore, the fact that the age of the oldest stars is roughly equal to the inverse of the Hubble constant emerges naturally from a Big Bang cosmology, but is an unexplained coincidence with most tired light models. |
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Among [[nonstandard cosmologies]] a few models addressing also the above criteria produce tired light redshift as a consequence of comprehensive theoretical treatments including i.a. [[time dilation]], and without referring to specific mechanisms.<ref>D.F. Crawford, ''Photon Decay in Curved Space-time'', [[Nature (journal)|Nature]], 277(5698), 633-635 (1979).</ref><ref>[[C. Johan Masreliez]], ''[http://www.estfound.org/downloads/pioneer_paper.pdf] The [[Pioneer Anomaly]]'', preprint. (2005) [[Astrophysics & Space Science]], v. 299, no. 1, pp. 83-108</ref> Lorenzo Zaninetti has described a static universe where the redshift is not due to expanding space, invoking two redshift mechanisms.<ref>http://link.aip.org/link/?PHESEM/23/298/1</ref> |
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In 2008, Blondin et al. showed that even processes that take macroscopic amounts of time such as various elapsed times are slowed down by the same redshift factor as the light frequency at high redshift.<ref>[http://arxiv.org/abs/0804.3595 Blondin et al.: Time dilation in type IA supernovae spectra at high redshift]</ref> |
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In 2010, D.L. Mamas presented a theoretical model purporting to satisfy the above basic criteria and stressing the importance of not neglecting the effects of cosmic dust when sampling and interpreting the light characteristics of objects at high redshift.<ref>[http://link.aip.org/link/?PHESEM/23/326/1 Mamas, D.L.: An explanation for the cosmological redshift]</ref> |
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==Notes== |
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Latest revision as of 21:32, 12 December 2024
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Physical cosmology |
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Tired light is a class of hypothetical redshift mechanisms that was proposed as an alternative explanation for the redshift-distance relationship. These models have been proposed as alternatives to the models that involve the expansion of the universe. The concept was first proposed in 1929 by Fritz Zwicky, who suggested that if photons lost energy over time through collisions with other particles in a regular way, the more distant objects would appear redder than more nearby ones.
Zwicky acknowledged that any sort of scattering of light would blur the images of distant objects more than what is seen. Additionally, the surface brightness of galaxies evolving with time, time dilation of cosmological sources, and a thermal spectrum of the cosmic microwave background have been observed—these effects should not be present if the cosmological redshift was due to any tired light scattering mechanism.[1][2][3] Despite periodic re-examination of the concept, tired light has not been supported by observational tests and remains a fringe topic in astrophysics.[4]
History and reception
[edit]Tired light was an idea that came about due to the observation made by Edwin Hubble that distant galaxies have redshifts proportional to their distance. Redshift is a shift in the spectrum of the emitted electromagnetic radiation from an object toward lower energies and frequencies, associated with the phenomenon of the Doppler effect. Observers of spiral nebulae such as Vesto Slipher observed that these objects (now known to be separate galaxies) generally exhibited redshift rather than blueshifts independent of where they were located. Since the relation holds in all directions it cannot be attributed to normal movement with respect to a background which would show an assortment of redshifts and blueshifts. Everything is moving away from the Milky Way galaxy. Hubble's contribution was to show that the magnitude of the redshift correlated strongly with the distance to the galaxies.
Basing on Slipher's and Hubble's data, in 1927 Georges Lemaître realized that this correlation could fit non-static solutions to the equations of Einstein's theory of gravity, the Friedmann–Lemaître solutions. However Lemaître's article was appreciated only after Hubble's publication of 1929. The universal redshift-distance relation in this solution is attributable to the effect an expanding universe has on a photon traveling on a null spacetime interval (also known as a "light-like" geodesic). In this formulation, there was still an analogous effect to the Doppler effect, though relative velocities need to be handled with more care since distances can be defined in different ways in an expanding universe.
At the same time, other explanations were proposed that did not concord with general relativity. Edward Milne proposed an explanation compatible with special relativity but not general relativity that there was a giant explosion that could explain redshifts (see Milne universe). Others proposed that systematic effects could explain the redshift-distance correlation. Along this line, Fritz Zwicky proposed a "tired light" mechanism in 1929.[5] Zwicky suggested that photons might slowly lose energy as they travel vast distances through a static universe by interaction with matter or other photons, or by some novel physical mechanism. Since a decrease in energy corresponds to an increase in light's wavelength, this effect would produce a redshift in spectral lines that increase proportionally with the distance of the source. The term "tired light" was coined by Richard Tolman in the early 1930s as a way to refer to this idea.[6] Helge Kragh has noted "Zwicky’s hypothesis was the best known and most elaborate alternative to the expanding universe, but it was far from the only one. More than a dozen physicists, astronomers and amateur scientists proposed in the 1930s tired-light ideas having in common the assumption of nebular photons interacting with intergalactic matter to which they transferred part of their energy." Kragh noted in particular John Quincy Stewart, William Duncan MacMillan, and Walther Nernst.[7]
Tired light mechanisms were among the proposed alternatives to the Big Bang and the Steady State cosmologies, both of which relied on the general relativistic expansion of the universe of the FRW metric. Through the middle of the twentieth century, most cosmologists supported one of these two paradigms, but there were a few scientists, especially those who were working on alternatives to general relativity, who worked with the tired light alternative.[8] As the discipline of observational cosmology developed in the late twentieth century and the associated data became more numerous and accurate, the Big Bang emerged as the cosmological theory most supported by the observational evidence, and it remains the accepted consensus model with a current parametrization that precisely specifies the state and evolution of the universe. Although the proposals of "tired light cosmologies" are now more-or-less relegated to the dustbin of history, as a completely alternative proposal tired-light cosmologies were considered a remote possibility worthy of some consideration in cosmology texts well into the 1980s, though it was dismissed as an unlikely and ad hoc proposal by mainstream astrophysicists.[9]
By the 1990s and on into the twenty-first century, a number of falsifying observations have shown that "tired light" hypotheses are not viable explanations for cosmological redshifts.[2] For example, in a static universe with tired light mechanisms, the surface brightness of stars and galaxies should be constant, that is, the farther an object is, the less light we receive, but its apparent area diminishes as well, so the light received divided by the apparent area should be constant. In an expanding universe, the surface brightness diminishes with distance. As the observed object recedes, photons are emitted at a reduced rate because each photon has to travel a distance that is a little longer than the previous one, while its energy is reduced a little because of increasing redshift at a larger distance. On the other hand, in an expanding universe, the object appears to be larger than it really is, because it was closer to us when the photons started their travel. This causes a difference in surface brilliance of objects between a static and an expanding Universe. This is known as the Tolman surface brightness test that in those studies favors the expanding universe hypothesis and rules out static tired light models.[10][11][12]
Redshift is directly observable and used by cosmologists as a direct measure of lookback time. They often refer to age and distance to objects in terms of redshift rather than years or light-years. In such a scale, the Big Bang corresponds to a redshift of infinity.[10] Alternative theories of gravity that do not have an expanding universe in them need an alternative to explain the correspondence between redshift and distance that is sui generis to the expanding metrics of general relativity. Such theories are sometimes referred to as "tired-light cosmologies", though not all authors are necessarily aware of the historical antecedents.[13]
Specific falsified models
[edit]In general, any "tired light" mechanism must solve some basic problems, in that the observed redshift must:
- admit the same measurement in any wavelength-band
- not exhibit blurring
- follow the detailed Hubble relation observed with supernova data (see accelerating universe)
- explain associated time dilation of cosmologically distant events.
A number of tired light mechanisms have been suggested over the years. Fritz Zwicky, in his paper proposing these models investigated a number of redshift explanations, ruling out some himself. The simplest form of a tired light theory assumes an exponential decrease in photon energy with distance traveled:where is the energy of the photon at distance from the source of light, is the energy of the photon at the source of light, and is a large constant characterizing the "resistance of the space". To correspond to Hubble's law, the constant must be several gigaparsecs. For example, Zwicky considered whether an integrated Compton effect could account for the scale normalization of the above model:
... light coming from distant nebulae would undergo a shift to the red by Compton effect on those free electrons [in interstellar spaces] [...] But then the light scattered in all directions would make the interstellar space intolerably opaque which disposes of the above explanation. [...] it is evident that any explanation based on a scattering process like the Compton effect or the Raman effect, etc., will be in a hopeless position regarding the good definition of the images.[5]
This expected "blurring" of cosmologically distant objects is not seen in the observational evidence, though it would take much larger telescopes than those available at that time to show this with certainty. Alternatively, Zwicky proposed a kind of Sachs–Wolfe effect explanation for the redshift distance relation:
One might expect a shift of spectral lines due to the difference of the static gravitational potential at different distances from the center of a galaxy. This effect, of course, has no relation to the distance of the observed galaxy from our own system and, therefore, cannot provide any explanation of the phenomenon discussed in this paper.[5]
Zwicky's proposals were carefully presented as falsifiable according to later observations:
... [a] gravitational analogue of the Compton effect [...] It is easy to see that the above redshift should broaden these absorption lines asymmetrically toward the red. If these lines can be photographed with a high enough dispersion, the displacement of the center of gravity of the line will give the redshift independent of the velocity of the system from which the light is emitted.[5]
Such broadening of absorption lines is not seen in high-redshift objects, thus falsifying this particular hypothesis.[14]
Zwicky also notes, in the same paper, that according to a tired light model a distance-redshift relationship would necessarily be present in the light from sources within our own galaxy (even if the redshift would be so small that it would be hard to measure), that do not appear under a recessional-velocity based theory. He writes, referring to sources of light within our galaxy: "It is especially desirable to determine the redshift independent of the proper velocities of the objects observed".[5] Subsequent to this, astronomers have patiently mapped out the three-dimensional velocity-position phase space for the galaxy and found the redshifts and blueshifts of galactic objects to accord well with the statistical distribution of a spiral galaxy, eliminating the intrinsic redshift component as an effect.[15]
Following after Zwicky in 1935, Edwin Hubble and Richard Tolman compared recessional redshift with a non-recessional one, writing that they
both incline to the opinion, however, that if the red-shift is not due to recessional motion, its explanation will probably involve some quite new physical principles [... and] use of a static Einstein model of the universe, combined with the assumption that the photons emitted by a nebula lose energy on their journey to the observer by some unknown effect, which is linear with distance, and which leads to a decrease in frequency, without appreciable transverse deflection.[16]
These conditions became almost impossible to meet and the overall success of general relativistic explanations for the redshift-distance relation is one of the core reasons that the Big Bang model of the universe remains the cosmology preferred by researchers.
In the early 1950s, Erwin Finlay-Freundlich proposed a redshift as "the result of loss of energy by observed photons traversing a radiation field".[17] which was cited and argued for as an explanation for the redshift-distance relation in a 1962 astrophysics theory Nature paper by University of Manchester physics professor P. F. Browne.[18] The pre-eminent cosmologist Ralph Asher Alpher wrote a letter to Nature three months later in response to this suggestion heavily criticizing the approach, "No generally accepted physical mechanism has been proposed for this loss."[19] Still, until the so-called "Age of Precision Cosmology" was ushered in with results from the WMAP space probe and modern redshift surveys,[20] tired light models could occasionally get published in the mainstream journals, including one that was published in the February 1979 edition of Nature proposing "photon decay" in a curved spacetime[21] that was five months later criticized in the same journal as being wholly inconsistent with observations of the gravitational redshift observed in the solar limb.[22] In 1986, a paper claiming tired light theories explained redshift better than cosmic expansion was published in the Astrophysical Journal,[23] but ten months later, in the same journal, such tired light models were shown to be inconsistent with extant observations.[24] As cosmological measurements became more precise and the statistics in cosmological data sets improved, tired light proposals ended up being falsified,[1][2][3] to the extent that the theory was described in 2001 by science writer Charles Seife as being "firmly on the fringe of physics 30 years ago; still, scientists sought more direct proofs of the expansion of the cosmos".[25]
See also
[edit]References
[edit]- ^ a b Wright, E. L. Errors in Tired Light Cosmology.
- ^ a b c Tommaso Treu, Lecture slides for University of California at Santa Barbara Astrophysics course. p. 16. Archived 2010-06-23 at the Wayback Machine.
- ^ a b Peebles, P. J. E. (1998). "The Standard Cosmological Model". In Greco, M. (ed.). Rencontres de Physique de la Vallee d'Aosta. arXiv:astro-ph/9806201.
- ^ Overduin, James Martin; Wesson, Paul S. (2008). The light/dark universe: light from galaxies, dark matter and dark energy. World Scientific Publishing. p. 10. ISBN 978-981-283-441-6.
- ^ a b c d e Zwicky, F. (1929). "On the Redshift of Spectral Lines Through Interstellar Space". Proceedings of the National Academy of Sciences. 15 (10): 773–779. Bibcode:1929PNAS...15..773Z. doi:10.1073/pnas.15.10.773. PMC 522555. PMID 16577237.
- ^ Evans, Myron W.; Vigier, Jean-Pierre (1996). The Enigmatic Photon: Theory and Practice of the B3 Field. Springer. p. 29. ISBN 978-0-7923-4044-7.
- ^ Kragh, Helge (2019). "Alternative Cosmological Theories". In Kragh, Helge; Longair, Malcolm S. (eds.). The Oxford Handbook of the History of Modern Cosmology. p. 29. doi:10.1093/oxfordhb/9780198817666.013.4. ISBN 978-0-19-881766-6.
- ^ Wilson, O. C. (1939). "Possible Applications of Supernovae to the Study of the Nebular Red Shifts". The Astrophysical Journal. 90: 634. Bibcode:1939ApJ....90..634W. doi:10.1086/144134.
- ^ See, for example, p. 397 of Joseph Silk's book, The Big Bang. (1980) W. H. Freeman and Company. ISBN 0-7167-1812-X.
- ^ a b Geller, M. J.; Peebles, P. J. E. (1972). "Test of the Expanding Universe Postulate". The Astrophysical Journal. 174: 1. Bibcode:1972ApJ...174....1G. doi:10.1086/151462.
- ^ Goldhaber, G.; Groom, D. E.; Kim, A.; Aldering, G.; Astier, P.; Conley, A.; Deustua, S. E.; Ellis, R.; Fabbro, S.; Fruchter, A. S.; Goobar, A.; Hook, I.; Irwin, M.; Kim, M.; Knop, R. A.; Lidman, C.; McMahon, R.; Nugent, P. E.; Pain, R.; Panagia, N.; Pennypacker, C. R.; Perlmutter, S.; Ruiz-Lapuente, P.; Schaefer, B.; Walton, N. A.; York, T.; The Supernova Cosmology Project (2001). "Timescale Stretch Parameterization of Type Ia Supernova B-band Light Curves". The Astrophysical Journal. 558 (1): 359–368. arXiv:astro-ph/0104382. Bibcode:2001ApJ...558..359G. doi:10.1086/322460. S2CID 17237531.
- ^ Lubin, Lori M.; Sandage, Allan (2001). "The Tolman Surface Brightness Test for the Reality of the Expansion. IV. A Measurement of the Tolman Signal and the Luminosity Evolution of Early-Type Galaxies". The Astronomical Journal. 122 (3): 1084–1103. arXiv:astro-ph/0106566. Bibcode:2001AJ....122.1084L. doi:10.1086/322134. S2CID 118897528.
- ^ Barrow, John D. (2001). Peter Coles (ed.). The Routledge Companion to the New Cosmology. Routledge. p. 308. Bibcode:2001rcnc.book.....C. ISBN 978-0-415-24312-4.
- ^ Newton, Elisabeth (27 April 2011). "Prospecting for C IV at high redshifts". astrobites.org. Retrieved 4 November 2023.
- ^ Binney & Merrifield: Galactic Astronomy. Princeton University Press, ISBN 978-0-691-02565-0.
- ^ Hubble, Edwin; Tolman, Richard C. (November 1935). "Two Methods of Investigating the Nature of the Nebular Redshift". Astrophysical Journal. 82: 302. Bibcode:1935ApJ....82..302H. doi:10.1086/143682.
- ^ Finlay-Freundlich, E. (1954). "Red-Shifts in the Spectra of Celestial Bodies". Proceedings of the Physical Society A. 67 (2): 192–193. Bibcode:1954PPSA...67..192F. doi:10.1088/0370-1298/67/2/114.
- ^ Brown, P. F. (1962). "The Case for an Exponential Red Shift Law". Nature. 193 (4820): 1019–1021. Bibcode:1962Natur.193.1019B. doi:10.1038/1931019a0. S2CID 4154001.
- ^ Alpher, R. A. (1962). "Laboratory Test of the Finlay-Freundlich Red Shift Hypothesis". Nature. 196 (4852): 367–368. Bibcode:1962Natur.196..367A. doi:10.1038/196367b0. S2CID 4197527.
- ^ Smoot, George S. "Our Age of Precision Cosmology". Proceedings of the 2002 International Symposium on Cosmology and Particle Astrophysics (CosPA 02), Taipei, Taiwan, 31 May – 2 June 2002, pp. 314–325.
- ^ Crawford, D. F. (1979). "Photon Decay in Curved Space-time". Nature. 277 (5698): 633–635. Bibcode:1979Natur.277..633C. doi:10.1038/277633a0. S2CID 4317887.
- ^ Beckers, J. M.; Cram, L. E. (July 1979). "Use of the solar limb effect to test photon decay and cosmological redshift theories". Nature. 280 (5719): 255–256. Bibcode:1979Natur.280..255B. doi:10.1038/280255a0. S2CID 43273035.
- ^ LaViolette, P. A. (April 1986). "Is the universe really expanding?". Astrophysical Journal. 301: 544–553. Bibcode:1986ApJ...301..544L. doi:10.1086/163922.
- ^ Wright, E. L. (February 1987). "Source counts in the chronometric cosmology". Astrophysical Journal. 313: 551–555. Bibcode:1987ApJ...313..551W. doi:10.1086/164996.
- ^ Seife, Charles (28 June 2001). "'Tired-Light' Hypothesis Gets Re-Tired". Science. Retrieved 2016-06-03.
Measurements of the cosmic microwave background put the theory firmly on the fringe of physics 30 years ago; still, scientists sought more direct proofs of the expansion of the cosmos.